Alternating Current Circuits

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Miles Logan
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1 Alternating Current Circuits

2 AC Circuit An AC circuit consists of a combination of circuit elements and an AC generator or source. The output of an AC generator is sinusoidal and varies with time according to the following equation: Δu = ΔV max sin 2 ƒt = ΔV max sin wt Δu is the instantaneous voltage.. ΔV max is the maximum voltage of the generator. ƒ is the frequency at which the voltage changes, in Hz.

3 rms Current and Voltage The rms ( root-mean-square ) current is the direct current that would dissipate the same amount of energy in a resistor as is actually dissipated by the AC current. Imax Irms.707Imax 2 Alternating voltages can also be discussed in terms of rms values. Vmax u.707 V 2 max

4 Ohm s Law in an AC Circuit rms values are used when discussing AC currents and voltages. AC ammeters and voltmeters are designed to read rms values. Many of the equations will be in the same form as in DC circuits. Ohm s Law for a resistor, R, in an AC circuit V I R R,rms rms (Also applies to the maximum values of v and i.)

5 Resistor in an AC Circuit Consider a circuit consisting of an AC source and a resistor. The graph shows the current through and the voltage across the resistor. The current and the voltage reach their maximum values at the same time. The current and the voltage are said to be in phase.

6 Resistors in an AC Circuit The direction of the current has no effect on the behavior of the resistor. The rate at which electrical energy is dissipated in the circuit is given by 2 P ir where i is the instantaneous current. The heating effect produced by an AC current with a maximum value of I max is not the same as that of a DC current of the same value. The maximum current occurs for a small amount of time.

7 Power in an AC Circuit The average power dissipated in resistor in an AC circuit carrying a current I rms is P ave 2 rms I R

8 Notation Note

9 Capacitors in an AC Circuit Consider a circuit containing a capacitor and an AC source. The current starts out at a large value and charges the plates of the capacitor.

10 Capacitors in an AC Circuit Consider a circuit containing a capacitor and an AC source. The current starts out at a large value and charges the plates of the capacitor. There is initially no resistance to hinder the flow of charge (current) while the plates are not charged.

11 Capacitors in an AC Circuit Consider a circuit containing a capacitor and an AC source; The current starts out at a large value and charges the plates of the capacitor. There is initially no resistance to hinder the flow of charge (current) while the plates are not charged. As the charge on the plates increases, the voltage across the plates increases and the current in the circuit decreases.

12 Capacitors in an AC Circuit The current reverses direction. The voltage across the plates decreases as the plates lose the charge they had accumulated. The voltage across the capacitor lags behind the current by 90.

13 Capacitive Reactance and Ohm s Law The impeding effect of a capacitor on the current in an AC circuit is called the capacitive reactance and is given by X C 2 1 fc When ƒ is in Hz and C is in F, X C will be in ohms. Ohm s Law for a capacitor in an AC circuit: V I X C,rms rms C

14 Inductors in an AC Circuit Consider an AC circuit with a source and an inductor. The current in the circuit is impeded by the back emf of the inductor. The voltage across the inductor leads the current by 90.

15 Inductive Reactance and Ohm s Law The effective resistance of a coil in an AC circuit is called its inductive reactance and is given by X L 2 fl When ƒ is in Hz and L is in H, X L is in ohms. Ohm s Law for the inductor: V I X L,rms rms L

16 The RLC Series Circuit The resistor, inductor, and capacitor can be combined in a circuit. At any instant, the current in the circuit is the same everywhere. The current varies sinusoidally with time.

17 Current and Voltage Relationships in an RLC Circuit The instantaneous voltage across the resistor is in phase with the current The instantaneous voltage across the inductor leads the current by 90 The instantaneous voltage across the capacitor lags the current by 90

18 To account for the different phases of the voltage drops, vector techniques are used. Represent the voltage across each element as a rotating vector, called a phasor. The diagram is called a phasor diagram. Phasor Diagrams

19 Phasor Diagram for RLC Series Circuit The voltage across the resistor is on the +x axis since it is in phase with the current. The voltage across the inductor is on the +y axis since it leads the current by 90. The voltage across the capacitor is on the y axis since it lags behind the current by 90.

20 Phasor Diagram Phasors are added as vectors to account for the phase differences in the voltages. ΔV L and ΔV C are on the same line and so the net y component is ΔV L ΔV C.

21 ΔV max From the Phasor Diagram The voltages are not in phase, so they cannot simply be added to get the voltage across the combination of the elements or the voltage source V V V V max tan V 2 2 R L C is the phase angle between the current and the maximum voltage. The equations also apply to rms values. L V V R C

22 The impedance, Z, can also be represented in a phasor diagram. 2 Z R X L X C tan X L Impedance of a Circuit 2 R X C

23 Phasor Applets

24 Impedance and Ohm s Law Ohm s Law can be applied to the impedance. ΔV max = I max Z This can be regarded as a generalized form of Ohm s Law applied to a series AC circuit.

25 Summary of Circuit Elements, Impedance and Phase Angles

26 Problem Solving for AC Circuits - 1 Calculate the inductive an capacitive reactances, X L and X C. Be careful of units use F, H, Ω Use X L and X C with R to find Z. Find the maximum current or maximum voltage drop using Ohm s Law, V max = I max Z

27 Problem Solving for AC Circuits - 2 Calculate the voltage drops across the individual elements using the appropriate form of Ohm s Law. Obtain the phase angle.

28 Power in an AC Circuit The average power delivered by the generator is converted to internal energy in the resistor: P av rms R rms rms cos I V I V cos is called the power factor of the circuit. Phase shifts can be used to maximize power outputs.

29 Resonance in an AC Circuit Resonance occurs at the frequency, ƒ o, where the current has its maximum value. To achieve maximum current, the impedance must have a minimum value. This occurs when X L = X C Then, f o 2 1 LC

30 An AC transformer consists of two coils of wire wound around a core of soft iron, The side connected to the input AC voltage source is called the primary and has N 1 turns. Transformers

31 Transformers The other side, called the secondary, is connected to a resistor and has N 2 turns. The core is used to increase the magnetic flux and to provide a medium for the flux to pass from one coil to the other. The rate of change of the flux is the same for both coils.

32 The voltages are related by N V V N1 Transformers When N 2 > N 1, the transformer is referred to as a step up transformer. When N 2 < N 1, the transformer is referred to as a step down transformer.

33 The power input into the primary equals the power output at the secondary: I 1 ΔV 1 = I 2 ΔV 2 (Conservation of energy) Transformers This assumes an ideal transformer. In real transformers, power efficiencies typically range from 90% to 99%.

General Physics (PHY 2140)

General Physics (PHY 2140) Lecture 10 6/12/2007 Electricity and Magnetism Induced voltages and induction Self-Inductance RL Circuits Energy in magnetic fields AC circuits and EM waves Resistors, capacitors